Observations of the nuclear region of the Seyfert galaxy NGC 4151
have been carried out at the Crimean Astrophysical Observatory with the 1.25 m
telescope using an aperture 20 arcsec in diameter.
Over 96 nights, 8 observational runs were made between
February 11, 1989 and June 14, 1996. We performed more than 1500 measurements in each of 5 spectral bands of Johnson's UBVRI system
simultaneously.
One measurement consists of 8 integrations of 10 s each. Photon
statistics corrected for sky background are applied to calculate
photometric errors, which were taken to be the same as the rms errors
obtained by averaging eight integrations. Taking into account the noise
variations of sky background and of a comparison star, we derived the
following rms errors for a single observation in the UBVRI bands,
respectively: 0
011, 0
006, 0
007, 0
007 and 0
004.
About 50% of observational nights lasted more than 1 hour; the longest
intranight observational run lasted 7.3 hours. The circumstances of the
observations were discussed in detail by Merkulova et al. (1999a,b).
The light curves of NGC 4151 in each of the UBVRI bands consist of
a slow increase of intensity over almost all the observing time, with
10-150 day outbursts superimposed on it (see Fig. 1). The increase of the
nucleus brightness began in February, 1990. The extraordinary long-term
brightening continued until June, 1996. The amplitudes of brightening
and gradients decreased from the U to the I band. The amplitudes amounted
to
2
2, 1
5, 0
9, 0
8 and 0
7 in the UBVRI bands, respectively.
The variability in the I band was at the level of about 10% per year.
Observations obtained in 1997-98 with Hubble Space Telescope using a
technique of high sensitivity and resolution of near-infrared imaging
detected variability of the NGC 4151 nucleus at 1.6
m at the same level:
11% over 7.3 months (Quillen et al. 2000).
The amplitudes of the UBVRI flux variability
/
for ten
day flares were 3.4, 1.8, 1.4, 1.4 and 1.3, respectively. The amplitudes of
intranight variations were as much as 15%. The amplitudes of all levels
of flux variability were significantly higher than the observational
errors.
A lot of the observational data permits us to search for the characteristics of the flux of the NGC 4151 nucleus variability with time, dividing all observational periods into four parts with a duration of 1.5-2.0 years as indicated in Table 1 and in Fig. 1. The duration of each period of time was defined approximately.
The columns of
this table show: (1) the number of periods of observation; (2) the
starting and ending Julian Dates of the period of observations
(JD = jd + 2400000 days); (3) the duration of the observations dt, days;
(4) the number of observational nights (n); (5) the number of
measurements (n1); (6) the power law spectral slopes of flux excesses
for I-IV periods of the nucleus brightening (
)
according to
Merkulova et al. (1999a).
Period | jd | dt, | n, | n1, |
![]() |
of observ. | days | days | nights | points | |
1 | 2 | 3 | 4 | 5 | 6 |
I | 47569-48216 | 648 | 18 | 190 | -1.17 |
II | 48216-48764 | 528 | 22 | 360 | -1.21 |
III | 48764-49479 | 522 | 10 | 167 | -0.90 |
IV | 49479-50249 | 764 | 46 | 841 | -0.37 |
Copyright ESO 2001